B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit

In the last decade a Quasi-Particle Model (QPM) has been developed to study charm quark dynamics in ultra-relativistic heavy-ion collisions supplying a satisfactory description of the main observables for D meson and providing an estimate of the space-diffusion coefficient Ds(T) from the phenomenolo...

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Main Authors: Maria Lucia Sambataro, Vincenzo Minissale, Salvatore Plumari, Vincenzo Greco
Format: Article
Language:English
Published: Elsevier 2024-02-01
Series:Physics Letters B
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269324000388
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author Maria Lucia Sambataro
Vincenzo Minissale
Salvatore Plumari
Vincenzo Greco
author_facet Maria Lucia Sambataro
Vincenzo Minissale
Salvatore Plumari
Vincenzo Greco
author_sort Maria Lucia Sambataro
collection DOAJ
description In the last decade a Quasi-Particle Model (QPM) has been developed to study charm quark dynamics in ultra-relativistic heavy-ion collisions supplying a satisfactory description of the main observables for D meson and providing an estimate of the space-diffusion coefficient Ds(T) from the phenomenology. In this paper, we extend the approach to bottom quarks describing their propagation in the quark-gluon plasma within an event-by-event full Boltzmann transport approach followed by a coalescence plus fragmentation hadronization. We find that QPM approach is able to correctly predict the first available data on RAA(pT) and v2(pT) of single-electron from B decays without any parameter modification w.r.t. the charm. We show also predictions for centralities where data are not yet available for both v2(pT) and v3(pT). Moreover, we discuss the significant breaking of the expected scaling of the thermalization time τth with MQ/T, discussing the evolution with mass of Ds(T) to better assess the comparison to lQCD calculations. We find that at T=Tc charm quark Ds(T) is about a factor of 2 larger than the asymptotic value for M→∞, while bottom Ds(T) is only a 20% higher. This implies a Ds(T) which is consistent within the current uncertainty to the most recent lattice QCD calculations with dynamical quarks for M→∞.
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spelling doaj.art-17f35275dcc94059a7036c0fd3a4a9a32024-02-05T04:30:48ZengElsevierPhysics Letters B0370-26932024-02-01849138480B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limitMaria Lucia Sambataro0Vincenzo Minissale1Salvatore Plumari2Vincenzo Greco3Department of Physics and Astronomy ‘E. Majorana’, University of Catania, Via S. Sofia 64, 1-95123 Catania, Italy; Laboratori Nazionali del Sud, INFN-LNS, Via S. Sofia 62, I-95123 Catania, Italy; Corresponding author.Department of Physics and Astronomy ‘E. Majorana’, University of Catania, Via S. Sofia 64, 1-95123 Catania, Italy; Laboratori Nazionali del Sud, INFN-LNS, Via S. Sofia 62, I-95123 Catania, ItalyDepartment of Physics and Astronomy ‘E. Majorana’, University of Catania, Via S. Sofia 64, 1-95123 Catania, Italy; Laboratori Nazionali del Sud, INFN-LNS, Via S. Sofia 62, I-95123 Catania, ItalyDepartment of Physics and Astronomy ‘E. Majorana’, University of Catania, Via S. Sofia 64, 1-95123 Catania, Italy; Laboratori Nazionali del Sud, INFN-LNS, Via S. Sofia 62, I-95123 Catania, ItalyIn the last decade a Quasi-Particle Model (QPM) has been developed to study charm quark dynamics in ultra-relativistic heavy-ion collisions supplying a satisfactory description of the main observables for D meson and providing an estimate of the space-diffusion coefficient Ds(T) from the phenomenology. In this paper, we extend the approach to bottom quarks describing their propagation in the quark-gluon plasma within an event-by-event full Boltzmann transport approach followed by a coalescence plus fragmentation hadronization. We find that QPM approach is able to correctly predict the first available data on RAA(pT) and v2(pT) of single-electron from B decays without any parameter modification w.r.t. the charm. We show also predictions for centralities where data are not yet available for both v2(pT) and v3(pT). Moreover, we discuss the significant breaking of the expected scaling of the thermalization time τth with MQ/T, discussing the evolution with mass of Ds(T) to better assess the comparison to lQCD calculations. We find that at T=Tc charm quark Ds(T) is about a factor of 2 larger than the asymptotic value for M→∞, while bottom Ds(T) is only a 20% higher. This implies a Ds(T) which is consistent within the current uncertainty to the most recent lattice QCD calculations with dynamical quarks for M→∞.http://www.sciencedirect.com/science/article/pii/S0370269324000388Relativistic heavy-ion collisionsQuark-gluon plasmaHeavy quark transportHeavy flavour hadronization
spellingShingle Maria Lucia Sambataro
Vincenzo Minissale
Salvatore Plumari
Vincenzo Greco
B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit
Physics Letters B
Relativistic heavy-ion collisions
Quark-gluon plasma
Heavy quark transport
Heavy flavour hadronization
title B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit
title_full B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit
title_fullStr B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit
title_full_unstemmed B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit
title_short B meson production in Pb+Pb at 5.02 ATeV at LHC: Estimating the diffusion coefficient in the infinite mass limit
title_sort b meson production in pb pb at 5 02 atev at lhc estimating the diffusion coefficient in the infinite mass limit
topic Relativistic heavy-ion collisions
Quark-gluon plasma
Heavy quark transport
Heavy flavour hadronization
url http://www.sciencedirect.com/science/article/pii/S0370269324000388
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